Transcript Chapter 18

Chapter 18
Direct Current Circuits
Sources of emf
• The source that maintains the current in a closed
circuit is called a source of emf
• Any devices that increase the potential energy of
charges circulating in circuits are sources of emf (e.g.
batteries, generators, etc.)
• The emf is the work done per unit charge
• SI units: Volts
emf and Internal Resistance
• A real battery has some internal resistance r;
therefore, the terminal voltage is not equal to the emf
• The terminal voltage: ΔV = Vb – Va
ΔV = ε – Ir
• For the entire circuit (R – load resistance):
ε = ΔV + Ir
= IR + Ir
emf and Internal Resistance
ε = ΔV + Ir = IR + Ir
• ε is equal to the terminal voltage when the current is
zero – open-circuit voltage
I = ε / (R + r)
• The current depends on both the resistance external to
the battery and the internal resistance
• When R >> r, r can be ignored
• Power relationship: I ε = I2 R + I2 r
• When R >> r, most of the power delivered by the
battery is transferred to the load resistor
Resistors in Series
• When two or more resistors are connected end-to-end,
they are said to be in series
• The current is the same in all resistors because any
charge that flows through one resistor flows through
the other
• The sum of the potential differences across the
resistors is equal to the total potential difference
across the combination
I1  I 2  I
V  IR1  IR2  I ( R1  R2 )  IReq
Resistors in Series
V  IReq
Req  R1  R2
• The equivalent resistance has the effect on the circuit
as the original combination of resistors (consequence
of conservation of energy)
• For more resistors in series:
Req  R1  R2  R3  ...
• The equivalent resistance of a series combination of
resistors is greater than any of the individual resistors
Resistors in Parallel
I1R1  I 2 R2  V
V V
I  I1  I 2 

R1
R2
• The potential difference across each resistor is the
same because each is connected directly across the
battery terminals
• The current, I, that enters a point must be equal to the
total current leaving that point (conservation of
charge)
• The currents are generally not the same
Resistors in Parallel
I1R1  I 2 R2  V
V V
I  I1  I 2 

R1
R2
1
1  V
 V    
 R1 R2  Req
1
1 1
 
Req R1 R2
Resistors in Parallel
• For more resistors in parallel:
1
1 1
1
   
Req R1 R2 R3
• The inverse of the equivalent resistance of two or more
resistors connected in parallel is the algebraic sum of
the inverses of the individual resistance
• The equivalent is always less than the smallest
resistor in the group
Problem-Solving Strategy
• Combine all resistors in series
• They carry the same current
• The potential differences across them are not
necessarily the same
• The resistors add directly to give the equivalent
resistance of the combination:
Req = R1 + R2 + …
Problem-Solving Strategy
• Combine all resistors in parallel
• The potential differences across them are the same
• The currents through them are not necessarily the same
• The equivalent resistance of a parallel combination is
found through reciprocal addition:
1
1 1
   ...
Req R1 R2
Problem-Solving Strategy
• A complicated circuit consisting of several resistors
and batteries can often be reduced to a simple circuit
with only one resistor
• Replace resistors in series or in parallel with a single
resistor
• Sketch the new circuit after these changes have been
made
• Continue to replace any series or parallel combinations
• Continue until one equivalent resistance is found
Problem-Solving Strategy
• If the current in or the potential
difference across a resistor in
the complicated circuit is to be
identified, start with the final
circuit and gradually work back
through the circuits (use formula
ΔV = I R and the procedures
describe above)
Chapter 18
Problem 13
Find the current in the 12-Ω resistor in the Figure.
Kirchhoff’s Rules
• There are ways in which resistors can be connected
so that the circuits formed cannot be reduced to a
single equivalent resistor
• Two rules, called Kirchhoff’s Rules can be used
instead:
• 1) Junction Rule
• 2) Loop Rule
Gustav Kirchhoff
1824 – 1887
Kirchhoff’s Rules
• Junction Rule (A statement of Conservation of
Charge): The sum of the currents entering any
junction must equal the sum of the currents leaving
that junction
• Loop Rule (A statement of Conservation of Energy):
The sum of the potential differences across all the
elements around any closed circuit loop must be
zero
Junction Rule
I1 = I2 + I3
• Assign symbols and directions to
the currents in all branches of the
circuit
• If a direction is chosen incorrectly,
the resulting answer will be
negative, but the magnitude will
be correct
Loop Rule
• When applying the loop rule, choose
a direction for transversing the loop
• Record voltage drops and rises as
they occur
• If a resistor is transversed in the
direction of the current, the potential
across the resistor is – IR
• If a resistor is transversed in the
direction opposite of the current, the
potential across the resistor is +IR
Loop Rule
• If a source of emf is transversed in
the direction of the emf (from – to +),
the change in the electric potential
is +ε
• If a source of emf is transversed in
the direction opposite of the emf
(from + to -), the change in the
electric potential is – ε
Equations from Kirchhoff’s Rules
• Use the junction rule as often as needed, so long as,
each time you write an equation, you include in it a
current that has not been used in a previous junction
rule equation
• The number of times the junction rule can be used is
one fewer than the number of junction points in the
circuit
• The loop rule can be used as often as needed so long
as a new circuit element (resistor or battery) or a new
current appears in each new equation
• You need as many independent equations as you have
unknowns
Equations from Kirchhoff’s Rules
Problem-Solving Strategy
• Draw the circuit diagram and assign labels and symbols
to all known and unknown quantities
• Assign directions to the currents
• Apply the junction rule to any junction in the circuit
• Apply the loop rule to as many loops as are needed to
solve for the unknowns
• Solve the equations simultaneously for the unknown
quantities
• Check your answers
Chapter 18
Problem 17
Determine the current in each branch of the circuit shown
in the Figure.
RC Circuits
• If a direct current circuit contains capacitors and
resistors, the current will vary with time
• When the circuit is completed, the capacitor starts to
charge until it reaches its maximum charge (Q = Cε)
• Once the capacitor is fully charged, the current in the
circuit is zero
Charging Capacitor in an RC Circuit
• The charge on the capacitor
varies with time
q = Q (1 – e -t/RC )
• The time constant,  = RC,
represents the time required for
the charge to increase from zero
to 63.2% of its maximum
• In a circuit with a large (small) time constant, the
capacitor charges very slowly (quickly)
• After t = 10 , the capacitor is over 99.99% charged
Discharging Capacitor in an RC Circuit
• When a charged capacitor is
placed in the circuit, it can be
discharged
q = Qe -t/RC
• The charge decreases
exponentially
• At t =  = RC, the charge
decreases to 0.368 Qmax; i.e., in
one time constant, the capacitor
loses 63.2% of its initial charge
Chapter 18
Problem 35
A capacitor in an RC circuit is charged to 60.0% of its
maximum value in 0.900 s. What is the time constant of
the circuit.
Chapter 18
Problem 54
An emf of 10 V is connected to a series RC circuit
consisting of a resistor of 2.0 × 106 Ω and a capacitor of
3.0 μF. Find the time required for the charge on the
capacitor to reach 90% of its final value.
Electrical Safety
• Electric shock can result in fatal burns
• Electric shock can cause the muscles of vital organs
(such as the heart) to malfunction
• The degree of damage depends on
– the magnitude of the current
– the length of time it acts
– the part of the body through which it passes
Effects of Various Currents
• 5 mA or less
– Can cause a sensation of shock
– Generally little or no damage
• 10 mA
– Hand muscles contract
– May be unable to let go a of live wire
• 100 mA
– If passes through the body for just a few seconds,
can be fatal
Answers to Even Numbered Problems
Chapter 18:
Problem 2
(a) 24 Ω
(b) 1.0 A
(c) 2.18 Ω, I4 = 6.0 A, I8 = 3.0 A, I12 = 2.0 A
Answers to Even Numbered Problems
Chapter 18:
Problem 6
15 Ω
Answers to Even Numbered Problems
Chapter 18:
Problem 18
5.4 V with a at a higher potential than b
Answers to Even Numbered Problems
Chapter 18:
Problem 22
0.50 W
Answers to Even Numbered Problems
Chapter 18:
Problem 36
(a) 10.0 μF
(b) 415 μC
Answers to Even Numbered Problems
Chapter 18:
Problem 38
(a) 8.0 A
(b) 120 V
(c) 0.80 A
(d) 5.8 × 102 W